Voice-operated signaling system



5 Sheets-Sheet l /NVENTOR R. C MTHES By ATTORNEY R. C. MATH ES TIME VOICE-OFERATED SIGNALING SYSTEM Nqv. 20, 1951 Filed sept. 21, 1949 Nov. A20, 1951 R. c. MATHEs y2,575,910

VOICE-OPERATED SIGNALING SYSTEM L 3/ L gnu- W7 /NVENTOR l?. CMTHES BYNMCW Nov. 20, 1951 R, Q MA1-HES 4 2,575,910

l VOICE-OPERATED SIGNALING SYSTEMy Filed Sept. 2l, 1949 5 Sheets-Sheet 3 /NVEA/rof? R. C. MA THES ATTORNEY Nov. zo, 1951 R. C. MATHS 2,575,910

VOICE-OPERATD SIGNALING SYSTEM Filed Sept. 21, 1949 5 Sheets-Sheet 5 FROM FIG.2

/NVENTOR /aa' R. C. MATHES A 7` TORNE V THRU THER RESET nELA rs /3 8 Patented Nov. 20, 1951 VOICE-OPERATED SIGNALIN G SYSTEM Robert C. Mathes, Maplewood, N. J., assignor to Bell Telephone Laboratories, Incorporated, New York, N. Y., a corporation of New York Application September 21, 1949, Serial No. 116,979

12 Claims. 1

This invention relates to voice-operated devices, and particularly to the selective actuation of mechanisms in response to the vocal pronouncement of a command word. It has for its principal object to render such actuation independent of the phonetic characteristics which distinguish one individual speaker from another .who pronounces the same word. Such apparatus may be employed in an automatic telephone exchange as a substitute for the present standard equipment which responds to the pulses generated by a finger dial.

It is known to analyze the sound of a spoken Word into its harmonic components and, when these components adopt a particular preassigned energy distribution, to actuate a mechanism such as a relay in response to the presence of this distribution. Thus, for example, Dudley Patent 2,238,555 shows a system in which the preassigned distribution of the harmonic components is one which corresponds to a single phonetic element, so called, i. e., one of a number of building blocks out of which it was once thought that all the Words of the English language could be constructed. Repetition of this action for the next phonetic element, and for the next, and so on, causes individual phonetic element relays to be actuated in a certain particular sequence and this, in turn, actuates a word relay. Such systems are open to the criticism that the distribution of the components of the sound of a given phonetic element differs from one individual voice to another, so that the apparatus responds diiferently to diiferent voices.

Recent Work as described by Potter, Kopp and Green in Visible Speech (Van Nostrand, 1947) shows that there are very definite energy-frequency-time patterns corresponding to dirferent words. These patterns delineate the movements on the frequency scale of the vocal cavity resonances as functions of time, i. e., as the word progresses from its inception to its termination. In the frequency range up to approximately 3009 cycles per second these patterns generally contain three significant resonances or bars which exhibit wide diilerences in shape and in location on the frequency scale from word to word. Such energy-frequency-time patterns, or spectrograms, as they have come to be called, would serve well as standards or reference patterns for comparison with the corresponding components of an unknown word as spoken by an unknown voice, were it not for the fact that these spectrograms also exhibit variations from voice to voice for a given word. A study of the spectrogram patterns for a large number of words as spoken by widely diierent voices reveals the fact that the principal variations from voice to voice are of two kinds: an expansion or contraction along the time scale which is due to Variations in talking speed, and a spreading or shrinking along the frequency scale which is associated with variations in the fundamental pitch of the voice. Both of these variations, taken together or separately, may be visualized as the result of imprinting the spectrogram of a word as spoken by a rapid. lowpitched voice onto a sheet of elastic material such as rubber, which is then stretched in either or both of two perpendicular directions. Stretching in one direction corresponds to drawing out the word in time, as with a slow talker. Stretching in the other direction corresponds to raising the resonance frequencies represented by the several bars. In this analogy all parts of the elastic sheet are proportionately stretched, whereas in the actual case the bars may be unequally shifted in frequency and the drawing out in time may be greater at one part of the Word than at another.

Accordingly, it is a specic object of the invention to obscure the effects of reference pattern variations from voice to voice: in other words, to normalize the comparison process in frequency and in time, and to carry out these two kinds of normalization independently, and separately or p together as required. This process, termed normalization in frequency and in time, involves modifying either the unknown signal or the reference standard signal. In the illustrative embodiments described below, frequency normalization is applied to the unknown while time normalization is applied to the standard. In brief, the sound of the unknown spoken word is analyzed and from this analysis signals are derived which are indicative of the frequencies of the several bars. At the same time a control signal is derived from the fundamental pitch of the voice, and this control signal is utilized to modify the several bar signals in reciprocal relation to the fundamental pitch, thus removing from the bar signals those variations which are associated with variations of pitch. The resulting frequency-normalized bar signals are then compared with standard reference space patterns in which the characteristics of a standard reference `word are stored by virtue of the fact that the shapes of the space patterns, in rectangular or polar coordinates, are conformable to the shapes of the resonance bars of the standard word as spoken 3 by a standard voice at standard speed. In one embodiment the comparison is made by deriving a standard time signal or pattern from each standard space pattern and balancing it on a time basis against the corresponding spoken word bar signal. In another embodiment the standard reference space pattern takes the form of a target path. or mazewhile the frequency-normalized bar signal controls a-fcursor vsuch as` avcathode beam, which attempts to trace this path under the combined influence of the bar signal and an advancing force. In eithercase,v imbalance or mismatch between the standard and the unknown modies the speed-Lofadvance 'inva sense to minimize the mismatch. "Thusinthewcase-oi the beam, its advance is accelerated 'or retarded as required, to enable it if possible to. trace or 4 from the bottom. This particular analysis is for the voiced vowel sounds in the digit ve.

The operation of the equipment may be regarded as taking place in two stages; first, the analysis of the incoming speech signal to derive certain control currents dening the bars of Fig. 1, and second, the use of these control currents in matching Vthe characteristics igof lthe incoming "signal against standardifreference patterns.

Ytion with Fig. 2, and the second in connection 4with Figs. 4 and 6.

In Fig. 2f speech energy originating, for example,:ingatelephone transmitter I, appears on track the target path from end to end. The acceleration and retardation of the advance of 'the beam or of the space pattern, as the case may be, are made tovdepend onv the speed with-which the matching `process proceeds. f Thusv -the Vreference -'standard is electivelynormal-ized in time, and an -elastic timefmatchhbetween it andltheunknown word-is achieved. I Y

It -is-a Yfeature of the invention that the rindividualresonances of the unknown voiceare ysegregated and treated individually, even thoughfor short intervalsone suchresonance vmay `shift Vto a part of the frequency-scale which isrordinarily occupied by another.

-v Other objects and ieatures, andthe manner in whichtheyare realized, will lbevapparent from `tlflie following detailed description of illustrative y embodimentsof the invention, .when considered` in-connection withthe drawings; in which:

' Fig. 1 is apart ofv a spectrogram ofthe word Fig. 2.is.,a block schematicdiagram of a resonance analyzerincludinga..correction circuit for.. thepitch of an individuals voice;

Fig. 2a is a Schematic circuit diagram showing the details of parts of Fig. 2;

Fig. 3 shows on an enlarged scale the ,second bar, ofFig. 1,` together with other curves of faster @onslowcr talkers use d in explaining the method of operation orobtaining an elastic timematch;

lifig.4 4 shows in diagram form the use of a refi erencepattern for generating a reference Ycurrent Vfor matching purposeswith the rate of generation controlled by feed-back circuits;

Fig. `5 illustrates the elasticV time-matching principle asapplied to targets in a cathode ray tube `Figj6 shows in diagram form the use of a I -7; and

Fig. 8 shows the relation which` holds between voice resonance bar frequencies and the fundamental pitch of the voice.

The sample analysis pattern shown-.inV Fig.V 1

Las recorded by a sound spectrograph shows Vgraph-v ically how the areas ofV high energy, the dark tareas, move about relative to the vertical frequency scale with the progress of time. 'From their appearance in these rpatterns these. dark ,areas are called bar I, bar. 2, andbar 3 counting f aleadla. Partotthe speech energy is taken off over lead 2to astandard amplier-rectier 3 such asgisordinarily used in echo-Suppressors or volume control circuits. It provides a direct-cur- -rent-out-put over lead l to actuate a start control as will be explained below in connection with Partv of. the..speechenergy` is taken over lead. 5 to a pitch detectioncircuitl. ForY thesuccessful practiceof this inventionitiwill. be suiilcientuif the. pitch detection Acircuit produces .aslowly fluctuating unidirectional voltage, .the amplitude of whichis at all times .substantially glinearly 1related tothe ,fundamentalirequency of .the signal Such pitch detecting" Ycircuits `are' well known.. and are, shown, ior.; example, ,in-'H. Dudley Patent 2,1 510 91.

The speech signal is alsodedover leadsl.V fxand 6 to three filters l, l and 1, whichnominally ypass the bandso to `'7.90 cycles, 7.00.to 2160 cycles,

and above 2100 cycles. These are` approximately the regions in Whichthe rst,fs econ d, and1 third resonances of the voice aremost commonly found. As will be explained below', provision is made for shifting these v division points to: meet' the: exceptional variations from this general rule.

The outputs from these filters gointurn Yto the vllflfli'lelfs 8, 8. and 8 andthe discriminatorsi/B,

9 and 9" which serve as frequency modulation detectors. The outputs of ,theseV detectors are slowly undulating unidirectional currentsawhose magnitude are proportional to the frequencies of the harmonic components oi greatest amplitude in the several lter outputs. and hence measure closely the locations, on the frequency scale,.of

the resonance in the speech signal. Other standard forms ofA F. `M. detectors, such `as pulse counters orY ratio detectors, may be used inplace of the-discriminators shown.

Parts of the outputs of the -detectorsrand' are combined in an adder I0 comprising. `buffer resistances I8 feeding .currents through vare sistor I9 `and thus providing input voltage to an amplier l1, whose output is fedback as ar control current over lead ll. Likewise `the outputs of the frequency modulation detectors Sand 97 arey similarly combined in a similaradder JIJ' to provideY a feedback control currentox/ er-r lead l I'. These control currents have amplitudesproportionalto the'average of theiirst and Ysecond voice `resonance frequencies -andto .the average of `the `second .and third voiceresonanceirequencies, respectively.

These control currents serve tomodifythe cut- 1 off frequencies of the filters 1, 1', 1, to take care of shiftsV of the voice resonancesbeyond vthe regions in which they are normally found;` f Thus the second resonance mayqoccasionally yfall below 700 cycles, in which case theA first resonance is still lower. Or the liirst; resonancezmayrocca- ,75 s ionally rise ,above 700 cyclesiingwhich; lIza-Scythe second resonance is still higher.4 By employing the control currents to maintain each of the filter cross-over points at a value approximately equal to the average of theresonance locations, each group of resonance energies is sent to its proper F. M. detector. `Similar considerations hold for the cross-over between the second resonance and the third.

There are a variety of means for varying the cut-off frequencies of the filters l, l', 'I" which select the three bands in which the three voice resonances are measured; i. e., for tracking these resonances. The means shown utilizes the control currents over leads I I and `I I to vary the magnitudes of the inductances or capacities of the filters, or both. For the present purposes the requirements are very approximate and no great precision is required in the control. Fig. 2a shows an expanded diagram of that part of Fig. 2 which is concerned with the adjustment of these filters by control currents over leads I I and I I'. A conveniently practical arrangement for the band pass filter l is to construct it of two filters in tandem, a high-pass filter having a nominal cut-ofi frequency of 700 cycles and a lowpass filter having a nominal cut-off frequency of 2100 cycles. Thus in Fig. 2a, filter l is shown as low-pass, one-section, mid-series-terminated lter consisting of two series arm inductances and one shunt arm capacitance, filter 'I' as a similar low-pass filter in tandem with a high-pass, onesection, mid-series-terminated filter consisting of two series capacitances and one shunt inductance, and filter l as a similar high-pass filter.

In all of these filters the reactance element which is varied by the control current is shown as `the inductance element. Each of the elements comprises a ferro-magnetic core 3D bearing in ductance windings 3| and a control winding 32. The control current over lead II passes through a resistor 33 in the input grid circuit of a pentodc 34. The output current of the pentode 34 passing through this control winding 32 produces a varying direct-current magnetization in the whole core 3U. As the magnetization approaches satul ration, in the case of materials such as Permalloy, the effective permeability varies inversely as the square of the magnetizing current. Thus the inductance of windings on the outer arms of the core varies inversely as the square of the control current, and hence the filter cut-off varies in direct proportion to the current from the pentode,

and hence, as the average location of the lower two resonance bars shifts toward higher frequencies the cut-off points of the low-pass filter 'l and the high-pass section of the filter 1 are shifted `upward in proportion. Similiarly the high-pass filter l and the low-pass part ofthe fllterl move up or down on the frequency scale `in direct relation to the average measured locations of the second and third resonance bars. No great precision is required in the control of these filter cut-offs, the only requirement being that the two sets of cross-overs lie between the two major resonances by pairs.

The inductance changes described above also result in changes `in the lter impedances and therefore in reflection losses. With appropriate lter terminations these are of negligible effect. As a refinement, they may be compensated by controlled alteration of the capacitance values of the filter condensers, the capacitance varia tions being so correlated with the inductance variations as to hold the filter impedances constant.

For this purpose` any :suitable voltage. or currentcontrolled capacitance may be employed. The so-called reactance tube is a familiar example.`

In addition to the direct method of controhthe filter transmission band edges may be shifted by the well-known heterodyne methods of shifting the signal location with respect to a fixed filter by double modulation. In this process the speech signal frequencies are shifted as a side band on a carrier frequency by a balanced modulator up to some convenient region say around l5 or 30 thousand cycles, where a fixed filter is located. The cut-off point of this filter with respect to the signal frequencies is then readily shifted by changing the carrier frequency under the control of the feedback currents on leads Il and II. Then by beating the signal back down to its original frequency band with the identical controlled carrier used to shift it up, it will appear as though the signal had passed through a variably controlled filter. This is the method commonly employed in many measuring instruments of the class known as frequency analyzers.

The discriminator outputs appearing on leads I2, I2 and I2 are proportional to the magnitudes of the frequencies denoting the locations of the three major resonances in the speech signal. As already indicated, these are proportionately higher for a female voice than for a male voice, for a sound having the same meaning. To correct this discrepancy and to bring the output currents to a common standard for voices of different pitches, use in made of the output of the pitch detecting circuit I3. This is led over a lead I4 to the three variable attenuation pads I5, I5 and I5. These pads may for example be simple T resistance pads with series arms of resistances 20, 20' and 20 and with the shunt arms of four-terminal thermistors Zll, 2l and 2I through whose heater windings 22, 22 and 22" the control current from the pitch detector I3 is passed. Due to the non-linear character of the thermistor resistance changes, practically any desired relation may be established between the current entering the pads I5 by way of leads I2, I2 and I2 and those leaving the pads by way of leads I6, I6' and I6 as a function of the control current which is in turn proportional to the fundamental pitch of the speech signal. The wide variations in these relations which are obtainable with thermistors are discussed in Properties and Uses of Thermistors by J. A. Becker, C. B. Green and G. L. Pearson, published in volume 26 of the Bell System Technical Journal, page (January 1947) Experience shows that the variation in the third bar frequency is about thirty per cent for an octave increase in the fundamental pitch, the second and rst bar variations being somewhat less. The necessary controls to compensate for these relations, which are depicted in Fig. 8, are easily obtainable with the aid of thermistors.

Accordingly, at the output of the circuit of Fig. 2 there are made available four control currents, a starting current and three control currents B1, B2, and Bz, proportional respectively to the resonance bar locations of the voice as normalized to a common standard pitch to allow for physical differences between talkers. p

The method and means chosen to illustrate the performance of the final function of pattern matching may best be approached by referring to Fig. 3 for bringing out the kind of problem involved. For this purpose it is sufficient to consider the time pattern for a single resonance.

'u The one selectedporresponds approximately to aangaat @par twofnof'rig: In thisafngure'tne abscissais timeand the-ordinate-is -trlequency'- (or the value offl theA control fourren't. proportionall to it) The curvelimaybetaken as ftheaverage value of .the resonanceJshiit--vwithfftime fora-'group 0I" talkers who pronounce this word. at` a certain ratelfintime, e.. g. ythemedianr .The curves Y5| and V52. are thelimitiineswithin' which Vthe .patterns forfallthese .talkers fall, the curvetubeing thetfrequency-time curveiof this resonance toria .particular one.;of `these `talkers contributingto the average.. Theareabetween.curves. 5i and 52 maythusj be takenas a. reference .pattern forV .this particular'reasonance.in a particular Word. .Patterns for the other two resonances areisirnilthericurves 5l, 52 denethe .reference pattern.

Therdotted curve 54 is ora-rapidtalker and the dot-dash curve 55 is for a. slow talker.V Both howeverare of the sameshapegas the pattern in the y'sense that-successive amplitude changes follow each other in` the same order in allV three cases. Y

It isa feature ofi-this invention that itprovides a solution to the problem of matchingtheincoming patternV against the reference pattern by iiexiblyshifting the time scales ofthe two patterns with reference to eachother in dependence on thedegreeY and direction ofk mismatch encountered. The mismatch generates a control current which is fed back to accelerate orfretard the rate vof comparison. Y

4"Iwo systems are shown by which the rate at which the comparison is made may be varied. In the rst of thesethe average value of the y pattern is .utilized ,to generate a current proportional tothe ordinate of the pattern, and this current is balanced against or subtracted from the incoming signal current. While many physicalmeans might be used'for generating a reference current proportionalto agraph such the line 50 of Fig.'3,`th'e'rst of these willbe explained in terms of a simple mechanical'illustration shown in Fig. 4. Cams 65, 5d @Ware driven by a shaftZ coupled to a variable 'speed directcurrent shunt-wound motor tilVV through a mag netic friction 'clutch S3. Theshape ot thercam is simply a polarrplot of'rthecurve 55 of Fig. 3. The cams 663' are similarly'shaped'to the polar forms of the rst and third resonance bars of Fig. 1. Also, each cam bears a contact-operating sector @e for establishing the conditions of operation in the table explained below and va terminating contactor 5.5 set in insulating disk/55.

The operation Vot the apparatus Yis initiated by the starting control currenton lead d Vfrom Fig. 2 which operates a relay 61 closing 'Contact 68 which, by way of a normally closedi'contact -69 and a leadr'lll, actuates the'magn'etic clutch VS3 and starts the shaft E2' rotating-atV the normal Y Vspeed of the motor @l which rotates continuously. lin one direction at apreassignedaverage speed.

As the cam 6D rotates, itdrivesf a contact point 1l', by way ofa push ro'd 12, up and down a potentiometer 13 supplied by a battery 'is with? a steady current. At the-same time push'rods 12 and 12" actuate potentiometers i3 and 13 under the action of camsil,l 60". Allactions and circuits fortheirst and third resonance bars-are indicated respectively" by numbers unprimedfand' double-primed, .'andfollow theqactions exactly as described for ithcsimilar primed:circuit ele.-

ments forthe secondbar of .Fig. 1..

'I'he .motion loffthe potentiometer contactipoint 1| thus generatesfia reference currentY which .bears the same functional.y relation to thelangle through which the shaft '62 has turned as` the ordinate of the curve 50 of. Eigbears to its abscissa..A L'Ihis control. current passes through .resistor Yl5 via resistor. '16'. `AtftheY same time the .signal control L current. toibe identied, car.-

ried Von the lead I 5 vof Fig. 2. and. .passed through. the resistor lfvia a resistor Y'lf'l' lin such 'polarity thatthe voltage developed 'across the :resistor 'I5' is proportional to the difference beitweenthe incoming signal currentand the ref- :erence current.; This difference currentpasses 4over lead i8 via thereversing switch contacts of relay 'I9' throughlwindings Bn and. Si oitwo rnarginal' polar relays,Y each biased.` off-contact. VAt this point, the three control .currents are averaged, by. virtuek of. the fact that the windings 8G, 8e and-.elffare allon the same relay,A as `are likewise the-windings 8l, 8 I and 8l.` When the relay imoperates,` due to a sufciently great 'average mismatch in onev direction of the' three reference currents as; compared to the three incorning'rsignalA currents, avoltage of one vpolarity .is carried from a battery 91 via lead `82 to an auxiliary field winding contained in the motor G-L'causing it to increase its speed, and forl an vunbalance in the reverse direction the relay SVI operates, connecting aYbattery-SS Yof the opposite sign to the lead 82 and thus causing the motor When the difference between the vtvvo currents exceeds the amount represented by the curves 5i and 52,- one of the marginalrelays 80 or 8-l is oper ated and the rate ofV generation of the reference current is accordingly altered. The direction in Ywhich the rate .of generationis to be altered may rnow be'seen by referringto Fig. 3. It will be seen that for a-rapid talker the curvey 54'intersects the upper limit curve 5I at a vpointfiiiA Where the slopes of the curves are positive; and this calls for increasing the rate of generation. of the reference current'to make for a better possibility of match .betweenit and the incomingvoice current. Also,

:slopes of theV curves .are positive they wouldintersect the lower limit curve 52 as atv aJpoint 58, indicating that a reduction of the rateo'f generation of a current proportional to the reference .pattern is `concerned wehave the following set of conditions: f Y Y Intersect Positive Slope n Y NegativeSlope Upper-limiti 4VAccelerate motor -r VDecelerate'motor. Lower limit Q.- Dece1erate'motor 'Accelerate motor.

As notedin the table of-.operating conditions K above `the function of increase-or. reduction of speed is reversed accordingly-as the slope of the reference .pattern curve i is .positive Vor .negative `at thev mismatch point. This function is AAtaken a care' oi'by the metallicsectorlid!fmountedion-the side of the camV En' and making contact with a Wiper 83" during that part of the revolution in which the slope of curve D on Fig. 3 is negative. That is, the edges 84', 85' of the sector 64' lie along radii of the cam 50' which mark the boundaries between the regions of positive and negative slope of the cam. When the cam has rotated so far that the edge 85 is opposite the push rod 12' and hence the push rod has reached its greatest travel, the sector 64 makes contact with the wiper 83' and, by operating the relay 19', reverses the polarity of windings 80' and 8| upon their respective relays. Thus the operating conditions of the table are carried out.

In case a resonance bar should have two or more maxima 0r minima instead of a single one as in Fig. 3, the corresponding angular areas of the cams may be provided with conductors 64 in greater numbers, accordingly.

If the shapes of the three incoming signal control currents, when thus elastically matched in time against a particular set of reference currents, permit one complete rotation of the shaft 62 in the speaking time of one word of the vocabulary the system is designed to recognize, then the contact 65 set in the insulating disk 86 makes contact with a wiper 86, thus completing the circuit of a battery 95 through the windings of relays 81 and 88, and through the contacts of relays 94, 94' and 94", to ground, and so actuating relays 81 and 88. Actuation of the load relay 81 closes a contact which permits the operation of the function desired corresponding to the particular word of the vocabularly, such for example assetting up a register in an automatic telephone exchange.

'I'he actuation of the reset relay 88 opens the contact 69 in the circuit of the magnetic clutch 63, uncoupling the shaft B2 from the driving motor 6|. During the rotation of the shaft, a tape 89 has wound up for one revolution on the outer face of the left'l hand member of the magnetic clutch against the pull of a coiled spring 98. Upon the release of the magnetic clutch `(i3, all three of the cams 68, 88', 89 are restored to their starting positions, determined by a limit stop 96, by the action of the spring 98, and the equipment is again ready to check for a match against another incoming word.

When the direction of mismatch is such that the motor is accelerated and the shaft completes one complete revolution ahead of the correct identification of the word being identied, the relays 94, 94', and 94" are provided to prevent the registration of a false identification and reset by this circuit. In this situation at least one of the three currents passing through the relays 94, 94' or 94" will have a value greater than the marginal operating current of these relays. Hence the operating circuit through relays 81 and 88 will be opened and the closing of contact 65 to Wiper 88 will be ineffective. In this case the system will be reset by a ground via one of the leads 93 from one of the other identifying equipment which correctly identifies this word.

Apparatus as above described is provided for each word of the designed vocabulary, and when any one of them has successfully matched the incoming signal, all must be reset for the next one. This is accomplished by the auxiliary contact 9| on the reset relay 88 which places a ground via lead 92 on the windings of each of the reset relays 88 on all the other equipments. The corresponding cross connections from all the other equipments are indicated by the multiple arrow 10 heads 93 coming in to place a ground on this relay 88.

As previously stated this mechanical cam is` only one physical means of generating a current proportional to the reference graph for carrying out the matching function. Electronic :means could equally well be used to generate a current having the required functional relations, for example in the manner shown in Sunstein Patent 2,461,667. In that case the control circuits may be applied to vary the speed of the sweep of a cathode beam as in this illustration they vary the speed of the motor.

In an alternative system for controlling the rate of comparison, a fixed reference space pattern is utilized as marked out by the lines 5| and 52 of Fig. 3, and an indicator is moved over this pattern under the control of the incoming speech signal current from each of the frequency detectors of Fig. 2 for the Vertical dimension and under the control of a variable driving rate for the horizontal dimension. While it is possible toconstruct such a system of mechanical elements, in this instance the invention will be illustrated by preferred systems employing electronic elements.

The central element of the electronic system is shown in Fig. 5 as comprising a target plate |10 in a cathode ray tube as the fixed reference space pattern upon which an electron beam 1| impinges as the moving indicator. The beam crossI section might be of conventional circular form but may preferably be of the elongated form as indicated by the spot |1I. The target |10 is shown as having the form of the reference pattern between lines 5| and 52 of Fig. 3. Back of the target plate |10 are four auxiliary target plates |12, |13, |14 and |15 upon which the beam impinges if it fails to follow the pattern of platee.

|18 as it is swept across. Reference to Fig. `3 will again show that if the rate of sweep is too slow the electron spot will leave the pattern plate to strike upon plates |12 or |13,and if the rate of sweep is too fast it will impinge on plates |14 or |15. Hence plates |12 and |13 are connected` normal rate of sweep of the spot across the pattern. If the spot is initially too low it will be subjected to `only a retarding force from the speed-reduction control over lead |10. Plate |12 is shown cut away for a short distance at the left so that if the spot is initially Well above the pattern'it will not receive a speed up control via lead |18. In fact, in one form of the invention as described below in connection with the complete circuit of Fig. 6, plates |12 and |13 may be omitted entirely. The final element in Fig. 5 is a small target |18 which the electron beam strikes if it successfully threads the maze set by the pattern plate. The electron current from this target is led out via lead marked reset as it serves to indicate the successful matching to this pattern and to reset all matching devices for the next word of command.

The pattern-matching operation will now be explained with reference to Fig. 6 in whichthe elements of Fig. 5 are shown similarly numbered as--theftargetsin a cathode ray tube'whose other elements are an enclosing envelope 9S, va cathode.`

|'U0,a f-control' electrodei el; an :accelerating and focusing electrode' itz;Y horizontal. 'deflection' plates"|03'and |4,and vertical deflection platesl [afstand-|06.. In matching patternsfor a Word, three-structures of this Ykind are used, as the shapesfof all three resonance patterns for a given WordmustV be substantially matched' by an -in-` comingilsignal Yfor its' identication. This may be donelwithlthree vseparate cathode ray tubes or,i.f:"preferred, three of -these structures may bev the-control elements |`U|` are biasedtoy a negative? potential-by la battery lill, no beam current iiovvs4 andY nothing happens; Action is initiated by thestarting`` current-from Fig. 2 on leads producing a' positive potential onv control lgrids l'l'l;= As this part of the circuit is at a high negative potential duetoffthe accelerating battery |98 of the beam tub'e, itumust dev this.v by indirectV means. TheV cntrolcurrent comingv in on lead iis used-to modulate any -convenient Asource |091 of -high V-frequency energy, Yby a carrier-elimination modu'jlater-I Ifll. The resulting alternating-currentsig-r nal is transmitted by a well insulated transform-'g er after'which it-is rectied by Yrectiiier-||2 and Vsmoothedbya condenser-I |-3 to produce a positive-potential on the electrodes lillv across a resistance |4.-- Each of the electronbeams, new

permitted to pass, reaches the target elements-at theirleftf side due tothe positivepotentialapplied- -tothe horizontal deiection plate ID3 by they battery ||5, and is drawn to the-bottoms of thet'arget array by the potential of a battery I |6 applied to the-'vertical plate |06.

If fatthe` samev time the control .current-B1* coming'by nway of lead Hij'frorml thefana'lyzer appara-tus'of Fig. Y2,V which represents the loca-- tion-of the iirst resonance, has the right value" forthis pattern, vit establishes a potentialfacrossv a resistor |17 which bringsthebeam up by the action-lof 'vertical deflection plate |05` until the spot |'1| strikes the pattern target |10 at its left end.

Y The electron beam current'collected' bythe pattern target |10, passing through a resistor'l I8A to'fground, provides an input `potential toa direct-V current amplifier i9 vwhose output current passes byvwayy of a buffer resistance through the commonresistance |2`| and to ground. The re.-y

sulting potential is further passed along through resistarices |22 and |23 to provide an input toA a summing amplifier |215;4 This amplifier isv biased to give zeroV outputl current until a positivespotential is applied to its input. When such potential is applied a proportionalcurrent 'o'ws througha large resistance |21 into a condenser |28'.` The' output of amplier |24 as its appears across VAthe'condenser |23 Vprovides thehorizontal deflection potential to plate |02 and also to the similar.v plates of the other structuresV for resonance patterns 2 and 3. The'time constant of the resistor |2f1and the condenser |28 is `set soV that for the duration of a single matching the voltageonl condenser |28 rises linearly with the product of current byt time. Thus for a constant input to ampli'er'lzd; the rate of sweep is @Qns The descriptionwill be given-'in vrespect agees/,91:01-

star-itl Similar inputscomebywayiot resistances Vbewadjusted to drivethe three spotszacross their:

respective patterns at a rate corresponding to. the normal ratel of speaking the word in question.:

Now,Jv as already explained inconnection with# Figs. 3 and 5, if the talker is pronouncingzthe particular word at a rate faster Ythan "averag'ef the beamfvvill move upward at a rate which carries: itupvvardwand onto the plate. |123Wh'os'e output; is now fed by way of the lead .|18 throughresiste' ance'- 29 to' ground, lproyiding an inputtoza directcurrent amplifier |30;r Theoutput oftheampliei iler V| Silr is adjusted by its Ibuffer,.resistance |31"` tuV make a much larger contribution 'tothe input: of amplier |22 thansithecontributicn: ofi the amplier" i I9.,- Hence the` sweep` will-.bef-.acceleratedY andl the spot'will iin'ifacttravelgalong.- imei pinging ppartly' cn thepattern"target"|10 andv partly on the back targeti 121i` Y If.' however,A the. iword is- Abeing Aspoken" more.,

- sluggishly" than normal, then'zthe. fspot will-.gc

on 'the targeti 1U; at itsA lower;boundary and part;- oft-he beanrcurrent` will 'go-to ground `throughresistance` |32 to provide'anfinputito a'directr@ currentzamplier 133;' ThisI amplifiers-has rits". outputrinverted, by: an--in'.ver-ter'stage' 140;' as compared'wth amplifiersv H92 and |`3ll.V Henceits` output subtracts from the input tothefamplier. l 24 andthe rate of sWeepfisLreduced; 1' Thelspot, then travels along partly on thep'a-ttern plate? 1| 10i and Vpartly on the-backfplateiil 14.-;rthef. degree vofV division of the spot being set byntherelative mage' nitudescf theoutput buiter resistancesf |20fand |34.:

As previously 'explained' f in .connection withl Figs `3 "and,I 5; they faction required; is reversed. wher'the spot intersects with a .negatively slop-r ing boundary 'as compared with a positively'slop-- ing one'. Hence back plate |1'5:fis"connectedf td back plate |14, so that either ofthem producesv deceleration. Similarly, back'pl'ate'sv |13and= |12/ are interconnected sov thateithenoffthem produ'cesf acceleration. If the resonance bar 'should have two or more maxima: or'minima, Atheb'ackv plates may be increased in number,"and interconnected accordingly. Y Y

By changing the relative magnitudes of resistances |22, |22" and '|22" it is possible'to weight the contributions of the three tracking controls to the inalsvveepV rate so that more importance may be given to one resonance'p'attern than to anotherin identifying a particular word. Thus for example,resonancernumber three for certain wordsmay 'be less constant in its characteristics Vfrom talker to talkerv than number one` or number two, and thus may be given less weight in the feedback control. A g

One equipment as described in Fig. 6 is needed foreach word in the command vocabulary and'. all may be supplied` simultaneously with the necessary control currents from the circu'itof Fig. 2. All will try to go into action at once when one-of the command Vwords is spoken. 'Some willnot start hunting across the pattern' at all as no spotY foh, one, two

incoming speech signal. With a suitably selected vocabulary, however, only one set of spots will traverse the whole pattern and the spots of this set will strike the targets |16, |16', |16". The beam currents passing to ground through resistance |35 then provide an input to a direct-current amplifier |36 whose output operates a load relay |31 and a group of reset relays |38, |38', |38. In some cases the mismatch may be such that the spots are swept at the accelerated rate to the end of the targets without holding a match. The margin of operation for relay |31 is set so as to operate only if beam current flows from all three of these targets. Hence if the beams are swept to the end of the targets without a match, relay |31 will not operateand hence an incorrect identification will not be given. The operation of the load relay |31 provides a contact closure in a local operating circuit which leads to the operation of any desired apparatus as required by the particular word in question. The group of reset relays |38', |38 etc. consists of one in each identifier corresponding to relay |38 whose operation discharges the condenser |28 through a relatively low resistance |39. Correspondingly, relay |38 is operated by auxiliary windings i4| by other identifier circuits. This restores `all tubes to their original conditions and the equipment is ready to receive the next word of command. Thus, even if two words arerun together with continuous voicing,` as soon as the first is identified the equipment is in readiness to proceed with the identification of the second. Where a single word is broken in the middle as by a stop consonant, it may be identified as two words, a pattern target being provided, along with associated circuits, for each half of the word.` For many purposes it is possible to use vocabularies of words not so broken. Thus the vocabulary nine contains only one such broken word; and this vocabulary suffices for a voice-operated telephone switching system.

The foregoing description has been given for the sake of generality, in terms of an embodimentwhich both accelerates and decelerates the speed of comparison. In some cases it will be possible to simplify the equipment and circuits by a relatively simple expedient which will next be described.

Suppose the outputs of the amplifiers connected to the pattern plates (amplifiers I I8 and plates 10 in Fig. 6) are set so that the rate of sweep established by them is somewhat greater than that required by the fastest talker. Then the only action required by a mismatch is to reduce the rate of sweep. This will occur automatically as the spot crosses the edge of the target due to the diminution of the amount of current to the target. A back plate may be used merely to drain off to ground that fraction of the beam current which misses the pattern plate. Back plates |12, |13, |14, and and all their associated amplilers and circuits may now be omitted. To facilitate the easy production of a range of sweep rates without hunting it is desirable, though not neces-f sary, to have a beam spot which is elongated vertically. Electron-optical systems for generating such a beam are well known. Or, the same effect may be secured by inserting a sawtooth source of high frequency in series with the bias on vertical deflection plate |06 which serves to cscillate the spot vertically over a small distance, say about `one-fourth to one-half thepattern plate width.

further simplification in the apparatus as illustrated in Fig. '7. The special tube structure i1- lustrated may be replaced by a standard cathode ray oscilloscope tube 200 of small size, having an internal fiuorescent screen 20| and an external opaque mask 202 placed over the end, of which a front view is shown in Fig. 7A. This mask is provided with a out out or open space of the same shape as the pattern matching plate |10 of Figs. 3 and 6. The light of the spot 203, caused by impact of the cathode beam on the screen 20|, is focused by lens 208 on a photoelectric cell 204 which takes the place of the resistance |8 as the input to the amplifier I I9 of Fig. 6, amplifiers |30 and |33 now being omitted from the circuit. This modified circuit now operates as for the single target plate. A front view of the photocell 204 is shown in Fig. 7B to have two electrically separate photosensitive areas 206 and 201. Light focused on the area 206, when the beam appears in the slot in the mask 202, provides the driving potential for the scanning over the greater part of the length of the slot. When the beam reaches the end of the slot, shown somewhat widened beyond the normal pattern to provide positive operation, the light is focused on area 201 which takes the place of target |16 in Fig. 6. Area 201 is connected into the circuit of Fig. 6, in place of resistance |35 to provide the input to the amplifier |36 for establishing the reset impulse. In all other respects the circuit operates as described in connection with Fig. 6.

Various other modifications will occur to those skilled in the art.

What is claimed is:

l. In a voice sound identifying system, in combination with a source of an unknown complex signal having a multiplicity of different frequency components, apparatus for identifying said signal which comprises means for deriving from said components a pattern representative of' the frequencies of energy maxima of said signal, a reference pattern similarly representative of the energy maxima of a standard signal, means for progressively comparing said first-named pattern with said reference pattern at a stand-ard speed, means for deriving a mismatch signal from said comparison, and means under control of said mismatch signal for varying the rate of comparison.

2. In a voice sound identifying system, a source of a signal which is an electrical counterpart of the complex wave form of a spoken word and which has a multiplicity `of different frequency components, means for deriving from said components a pattern indicative of the frequencies of energy maxima of said signal, a reference pattern similarly representative of the energy maxima of a standard signal, means for progressively comparing said first-named pattern with said reference pattern at a standard speed, means for deriving a mismatch signal from said comparison, and means under control of said mismatch signal for varying the rate of comparison.

3. In a voice sound identifying system, a source of a signal which is an electrical counterpart of the wave form of a spoken word, means for deriving from said signal a time pattern representative of the energy-frequency-time behavior of a voice-resonance of said word, a space pattern which is similarly representative of the behavior of the corresponding resonance of said word as `spoken by a standard Voice at standard speed, a pattern-tracing element, means for advancing This mode of operation makes possible'a still -said element along the time-dimension of said andere space patternat-an average-,speed means fordenectingcsaid element a1ongtne frequency dimension .of` said Vspace v,pattern under `control of said time patterns, means for deriving a correction sig- Y advance of said element under control of a departure of said element from said space pattern, and meansresponsive to a passage of-said element fromfend to endof said spacefpattern for generating anidentifcation signal'.

4'., In combination with a signal source, apparatuszfor identifying anunknown signal of said source which comprises a cathode beam tube having anelctrongun and a target having the configuration of a,Standardreference signal in fre- .quency-time coordinates, means for sweeping the beam ,along the target in the direction of the time coordinate at a variable speed, means for 4deflecting the beam across the target in the direction of the frequency coordinate under` control of`said unknown source signal, means vfor deriving a correction signal from departure of the beam from the target, connections Vfor ap- Y plying said correction signal to said beam-sweepl ing means to vary the speed of sweep, and means responsive to tracking of said target bysaid beam from end to end of saidtarget for generating an identification Y signal.

5,; In a voice-operated system, means for ,i

analyzing ,the progressive sound of a spoken word into groups of harmonic components, means for .selectinga principal one ofsaid components, the frequency of said principal component changing continuously, a cathode beam Vtube having an c electron gun and a target having a configuration related to the frequencyyof the corresponding component of a standard word as spoken by a `standard voice at standard speed, means for sweeping the. beam along the target in one direction at a variablespeed, means for delectingA the beam across the target in another direction under control vof the principal spoken word component, means for deriving a signal from departure of the `beam from the target, connections for applying said signal to said beamsweeping means to vary the speed of sweep, and

energies, the frequencies of said components;

changing continuously, means `for mutually l isolating Said selected components, a plurality of Vcathode, beam jtuoes each having .an electron gunand a-,vta-rget havinga conguration related tothe frequency fof Aone of said components of a `standard Yword Yas spoken by a vstandard voice at standard speed, means for sweeping the several jbeamsalong the severaltargets in one direction at a variable speed, means for defiecting each of the beams across itsl target'in another direction under control of one of the selected components, means for deriving a signal .from departure of each, vbeam from its target, means for averaging .said derived signals, connections'for applying said `signals as averaged to said beam-sweeping means -to vary the SpeedgOf Slvccpyand means responsive to tracking of lsaid targets by said beam from end to end goffsaidtargets for generating an ,identiviication signal.V Y

signal recognition apparatus-,which com- 16 prises a sourceci an illknownsgnal, a vcatl'iode beam-,tube havingan electrongun, a targethav-` ing a conigurationrelated toca desired charac,-

ofA `alstandard signal as generateclat a standardspeed,V means r,for sweeping `the beam alongythe/targetfin one direction atrga lvariable speedmeans,for ideflecting the beam across the target in another-direction under control of said unknown signal, means `for deriving a control signal from departure of said beam from said target, connectionsfor applying said'control sig-Y nalto,saidbeam-sweeping-means to 'vary the speed of sweep, andmeansresponsive to tracking oi-said target bysaid beam from end to end Y Y alongthe target in` one direction-at a variable speed; means for deriving vasweep-p-otential from impact: of 'said-'bearr-1fY mon `said :target-y means for applying `Said potential Vto said beam-sweeping means to generate'a sweep of average speed, means vforfzdeecting the beam across thertarget in anotlier'direction Yunder control of'saidfunknownsignaL means for derivinglacontrol signal -fromfdeparture of lsaid beam from said target, connections A for applying said control signal to said beam-sweeping means to vary the' speed :ofV

sweep,andrmeans responsive to tracking `of rsaid target ,by said beam yfrom zend Vto end thereof` for generating.anfidentication signal. Y A

'19. :Signal Vrecognition apparatus which comprises ka source cfa-n vunknown signal,` a cathode beam 'tube having an electron gun, a principal target *having a conguration related toa desired characteristic of a standard signalas'generat'ed'a-t -a standar-d speed, auxiliary targets disposedat the boundaries of said principal target, 'means vfor sweeping the 'beamalongthe principal targetin one directionat a variable speed',- means `for deecti-ng the beam across the principaltarget in another Ydirection under control of said unknown signal", ymeans for deriving a A`svi/ecp- Yretarding'signal lfrom V,impact of saidibeam on a forward boundary target, means for deriving l a sweep-accelerating signal from impact of said vbeam on .a rearward boundary'target, means for applying Asaid retarding signal and said accelerating signal to said 'beam-sweeping, means to vary the speed of sweep accordingly, and means responsive to tracking of said principal `target by said beam from end to end thereof for generating an identification signal.

10. `In a voice,A sound-identifying system, a source offa complex signal-which is an electrical Ycounterpart ofthe wave form .of a spoken word Aand which `has .a plurality of. diierent frequency components, rmeans for deriving `from said components a time pattern indicative of the energyfrequency-time relations of a principal voice .resonance Aof ,said spoken word, a space lpattern conforming tojthe energy-frequency-time diagram `ofa corresponding resonance of lsaid -word as spoken'by astandard voice at a standard speed, vmeans for advancing'said space patternat an avcragefspeed means orderiving frommovement of said space pattern avstandard time pattern 4proportional thereto, means 'for Vcomparing said `spoken*wordrtime pattern with saidV standard time pattern to derive a mismatch signal, means for fyarying fthesyspeed Lof Y advance; of said space pattern under control of said mismatch signal, and means responsive to movement of said space pattern through its full length, Without the derivation of a mismatch signal in excess of a preassigned threshold value, for generating an identicaton signal.

11. In combination with a source of a complex signal characterized by a plurality of different frequency harmonic components, apparatus for identifying said signal which comprises a relatively small number of filters having contiguous pass bands which together cover the frequency range of said signal, each such pass band being bounded by an adjustable cut-olf frequency, said lters having input terminals connected in parallel to said source, each of said filters having an output terminal, a discriminator connected to the output terminal of each lter for deriving a control signal which bears a preassigned relation to the frequency of an energy maximum of those components of said complex signal which are passed by the filter to which it is connected, and means for adjusting said cut-off frequencies by said control signals in a sense to maintain one of said energy maxima approximately centered in each of said pass bands.

12. In combination with a source of a complex signal characterized by a plurality of different frequency harmonic components of variable energy distribution, apparatus for maintaining the identity of the several energy maxima of said distribution which comprises a number of filters having contiguous pass bands which are adjustable on the frequency scale and which together cover the frequency range of said signal, the number of said filters being equal to the number of distinct energy maxima normally present in said signal, said filters being supplied in parallel by said source, a frequency-responsive element coupled to each filter, means for deriving an output signal from each frequency-responsive element, means for averaging the output signals of adjacent frequency-responsive elements by pairs to derive control signals, and feedback means for adjusting the out-off point separating the pass bands of two contiguous filters by the control signal derived from said two filters.

ROBERT C. MATHES.

REFERENCES CITED The following references are of record in the le of this patent:

UNITED STATES PATENTS Number Name Date 2,151,091 Dudley Mar.. 21, 1939 2,238,555 Dudley Apr. 15, 1941 2,293,203 Gosmann Aug. 18, 1942 2,413,263 Suter Dec.. 24, 1946 

